WO2022247851A1 - 波导光放大器 - Google Patents

波导光放大器 Download PDF

Info

Publication number
WO2022247851A1
WO2022247851A1 PCT/CN2022/094892 CN2022094892W WO2022247851A1 WO 2022247851 A1 WO2022247851 A1 WO 2022247851A1 CN 2022094892 W CN2022094892 W CN 2022094892W WO 2022247851 A1 WO2022247851 A1 WO 2022247851A1
Authority
WO
WIPO (PCT)
Prior art keywords
waveguide
gain
pumping
optical amplifier
light
Prior art date
Application number
PCT/CN2022/094892
Other languages
English (en)
French (fr)
Inventor
杨波
Original Assignee
珠海庞纳微半导体科技有限公司
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Priority claimed from CN202110593593.7A external-priority patent/CN113359232A/zh
Priority claimed from CN202121190000.4U external-priority patent/CN215813433U/zh
Application filed by 珠海庞纳微半导体科技有限公司 filed Critical 珠海庞纳微半导体科技有限公司
Publication of WO2022247851A1 publication Critical patent/WO2022247851A1/zh

Links

Images

Classifications

    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B6/122—Basic optical elements, e.g. light-guiding paths
    • G—PHYSICS
    • G02—OPTICS
    • G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
    • G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
    • G02B6/122—Basic optical elements, e.g. light-guiding paths
    • G02B6/125—Bends, branchings or intersections

Definitions

  • the application belongs to the technical field of optical amplifiers, in particular to waveguide optical amplifiers.
  • the optical amplifier is a basic optical device and one of the important optical devices for the miniaturization and integration of optical devices in the future. It is now widely used in the interconnection of optical devices and optical communication networks. However, the size of the current mainstream optical amplifiers is relatively large, which cannot meet the market demand and technical trend of miniaturization and integration of optical amplifiers.
  • a waveguide optical amplifier including:
  • the gain waveguide assembly includes a first gain waveguide and a second gain waveguide that are bent and connected, the first gain waveguide has an incident end, the second gain waveguide has an exit end, at least part of the first gain waveguide is close to at least part of the gain waveguide In the second gain waveguide, the transmission direction of the signal in the first gain waveguide is opposite to the transmission direction in the second gain waveguide;
  • the pumping waveguide covers at least part of the gain waveguide component, and at least part of the pumping waveguide covers the first gain waveguide and the second gain waveguide which are close to each other.
  • the gain waveguide component is used to transmit signal light
  • the pump waveguide is used to transmit pump light
  • the material of the gain waveguide component includes erbium-doped gallium nitride.
  • the material of the pumping waveguide includes gallium nitride and other group III nitrides.
  • the pumping waveguide includes a first part and a second part that are connected, and the first part covers the first gain waveguide and the second gain waveguide that are close to each other at the same time; the second part covers the rest respectively.
  • the first gain waveguide and the second gain waveguide are connected, and the first part covers the first gain waveguide and the second gain waveguide that are close to each other at the same time; the second part covers the rest respectively.
  • the first part covers one of the first gain waveguides and one of the second gain waveguides at the same time.
  • first gain waveguide and the second gain waveguide are arranged in a helical shape, and at least part of the second gain waveguide is arranged between adjacent first gain waveguides, and the incident end
  • the emitting end can be located on the same side or different side of the helical arrangement.
  • the pumping waveguides are also arranged in a helical shape, and there is a distance between adjacent pumping waveguides.
  • the opposite sides of the second gain waveguide are provided with a first gain waveguide M and a first gain waveguide N, and the second gain waveguide and the first gain waveguide M are set on the same pumping waveguide Inside, the second gain waveguide and the first gain waveguide N are set in the adjacent pumping waveguide; the distance between the second gain waveguide and the first gain waveguide M is smaller than the first gain waveguide M The distance between the second gain waveguide and the first gain waveguide N.
  • the incident end and the exit end are located on the same side of the helical arrangement, the incident end and the exit end are arranged at 90°, 180°, or 270° so that the incident light and the outgoing light Vertical arrangement; when the incident end and the exit end are located on the same side of the helical arrangement, the incident light and the exit light are arranged in parallel.
  • the distance between the first gain waveguide and the second gain waveguide covered by adjacent pumping waveguides is equal.
  • the incident end and/or the exit end may protrude from the pumping waveguide.
  • the pumping waveguide has a light-incident end and a reflection end oppositely arranged, and the waveguide optical amplifier also includes a reflection member, and the reflection member is arranged on the reflection end for reflecting the pump that arrives there. Pu Guang.
  • the waveguide optical amplifier further includes a coupler, and the coupler is respectively or simultaneously connected to the first gain waveguide, the second gain waveguide, and the pumping waveguide.
  • the pumping waveguide has a light-incident end
  • the waveguide optical amplifier further includes a pumping light source
  • the pumping light source is close to the light-incending end, and the pumping light of the pumping light source passes through the light-incident end of the coupler into the pump waveguide.
  • the transmission direction of the light emitted by the pump light source at the incident end in the pump waveguide is the same as the transmission direction of the signal light; the light emitted by the pump light source at the exit end is The transmission direction in the pumping waveguide is opposite to the transmission direction of the signal light.
  • the waveguide optical amplifier further includes a substrate, the gain waveguide component and the pumping waveguide are both arranged on the substrate, and the gain waveguide component and the substrate are further provided with the pump waveguide.
  • the substrate and the pumping waveguide may be of an integrated structure.
  • the waveguide optical amplifier further includes a coupler and a pumping light source, and the coupler and/or the pumping light source are also arranged on the substrate.
  • FIG. 1 is a schematic diagram of a waveguide optical amplifier in an embodiment of the present application.
  • Fig. 2 is a schematic cross-sectional view along the direction A-A in Fig. 1 .
  • FIG. 3 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • Fig. 4 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • FIG. 5 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • Fig. 6 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • FIG. 7 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • FIG. 8 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • FIG. 9 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • FIG. 10 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • Fig. 11 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • Fig. 12 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • FIG. 13 is a schematic cross-sectional view of a waveguide optical amplifier in another embodiment of the present application.
  • Waveguide optical amplifier-1 gain waveguide assembly-10, first gain waveguide-11, first gain waveguide M-111, first gain waveguide N-112, second gain waveguide-12, incident end-13, exit end- 14.
  • the optical amplifier is a key device in a high-speed optical communication system, and it is also one of the important optical devices for the miniaturization and integration of optical devices in the future.
  • Optical amplifiers include fiber amplifiers, waveguide optical amplifiers and other types of optical amplifiers.
  • the optical fiber amplifier uses rare earth doped optical fiber as the carrier of the amplifying medium.
  • the waveguide optical amplifier which can replace the optical fiber amplifier, has the characteristics of miniaturization and can be integrated on the chip. It has attracted more and more attention and research of scholars.
  • waveguide optical amplifiers can be divided into three modes: forward pumping, reverse pumping and bidirectional pumping according to the difference in the transmission directions of pump light and signal light.
  • forward pumping means that the pump light and signal light enter in the same direction, that is, the transmission direction is the same
  • reverse pumping means that the pump light and signal light enter from the opposite direction, that is, the transmission direction is opposite.
  • the bidirectional pumping is to inject a beam of pump light from the forward direction and the reverse direction, so that part of the signal light and the pump light have the same transmission direction, and part of the signal light and the pump light have opposite transmission signals.
  • the noise figure of the forward pump is small, but the saturation power is low, which is not conducive to the application of high output power.
  • the noise figure of reverse pumping is large, but the saturation power is high.
  • Bidirectional pumping can have the advantages of both at the same time, that is, small noise figure and high saturation power.
  • the waveguide optical amplifier can be divided into the core layer and the cladding layer surrounding it from the structural point of view.
  • the signal light mainly propagates in the core layer
  • the waveguide used as an optical amplifier can be divided into core layer pumping and cladding layer pumping according to the position of the pumping light.
  • the cladding pump can accommodate more pump light, so it has higher pump coupling efficiency.
  • adjacent waveguides Since there will be coupling crosstalk when adjacent waveguides are in contact, adjacent waveguides must be separated by a certain distance to ensure that they do not affect each other. Since the cladding waveguide where the pumping light is located is usually relatively wide, the spacing must be relatively large, resulting in a large size of the waveguide optical amplifier, which is not conducive to reducing the chip size.
  • FIG. 1 is a schematic diagram of a waveguide optical amplifier in an embodiment of the present application.
  • Fig. 2 is a schematic cross-sectional view along the direction A-A in Fig. 1 .
  • FIG. 3 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • Fig. 4 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • This embodiment provides a waveguide optical amplifier 1 , which specifically includes a gain waveguide component 10 and a pumping waveguide 20 .
  • the gain waveguide assembly 10 includes a first gain waveguide 11 and a second gain waveguide 12 that are bent and connected, the first gain waveguide 11 has an incident end 13, and the second gain waveguide 12 has an exit end 14, at least part of the The first gain waveguide 11 is close to at least part of the second gain waveguide 12 , and the transmission direction of the signal in the first gain waveguide 11 is opposite to the transmission direction in the second gain waveguide 12 .
  • the pumping waveguide 20 covers at least part of the gain waveguide assembly 10 , and at least part of the pumping waveguide 20 covers the first gain waveguide 11 and the second gain waveguide 12 which are close to each other.
  • the waveguide optical amplifier 1 provided in this embodiment includes a gain waveguide component 10, wherein the function of the gain waveguide component 10 is to transmit signals, that is, the gain waveguide component 10 can also be regarded as a core layer.
  • the gain waveguide assembly 10 is not composed of one kind of gain waveguide, but is composed of at least two kinds of gain waveguides, that is, a first gain waveguide 11 and a second gain waveguide 12 that are bent and connected. Or it can also be understood that the gain waveguide component 10 is a gain waveguide, but for the convenience of distinction, the waveguide is artificially named and distinguished from the bend according to its different functions.
  • the transmission direction of the signal in the first gain waveguide 11 is opposite to the transmission direction in the second gain waveguide 12, so the gain waveguides are distinguished according to whether the signal propagation direction is the same or not. That is, the first gain waveguide 11 and the second gain waveguide 12 have an integrated structure.
  • the gain waveguide assembly 10 is divided into a first gain waveguide 11 and a second gain waveguide 12 connected by bending, and at the same time, at least part of the first gain waveguide 11 is close to at least a part of the second gain waveguide 12, that is, a
  • the longer gain waveguide is bent into two sections of gain waveguide, thereby reducing the size occupied by the gain waveguide assembly 10 .
  • the transmission direction of the signal in the first gain waveguide 11 is opposite to the transmission direction in the second gain waveguide 12 (as shown in the D1 direction in Figure 1), which is the subsequent pumping waveguide 20 with the setup of the pump light to lay the foundation.
  • the waveguide optical amplifier 1 provided in this embodiment further includes a pumping waveguide 20 , so that the pumping waveguide 20 covers the gain waveguide component 10 .
  • the function of the pumping waveguide 20 is to cover and protect the gain waveguide component 10, so the pumping waveguide 20 can be regarded as a cladding layer.
  • the pumping waveguide 20 is also used to transmit pumping light, that is, the signal light is transmitted in the gain waveguide assembly 10, and the pumping light is transmitted in the pumping waveguide 20, so the waveguide optical amplifier 1 provided by this application can be regarded as is the cladding pump.
  • the role of the pump light is to provide additional energy to the signal light in the gain waveguide component 10 so that the signal light can be amplified.
  • the pumping waveguide 20 can simultaneously cover the first gain waveguide 11 and the second gain waveguide 12 that are close to each other.
  • the pump waveguide 20 only covers one gain waveguide (the first gain waveguide 11 or the second gain waveguide 12), and in order to prevent coupling crosstalk when adjacent waveguides are in contact, the adjacent pump waveguides 20 There will be a gap between them.
  • the present application uses the pumping waveguide 20 to cover the first gain waveguide 11 and the second gain waveguide 12 that are close to each other at the same time, even if the pumping waveguide 20 covers two or more gain waveguides at the same time, so the pumping waveguide 20 can be reduced.
  • the length of the pump waveguide 20 can also reduce the number of spaces between adjacent pump waveguides 20 and at the same time cover the space between the first gain waveguide 11 and the second gain waveguide 12 in the pump waveguide, thereby reducing waveguide light
  • the size of the amplifier 1 ultimately reduces the size of the chip. Because the pump waveguide 20 covers the gain waveguide with opposite transmission direction at the same time, a single pump light source can also realize bidirectional pumping, further reducing the size of the optical amplifier to meet the needs of users. In this embodiment, all the pumping waveguides 20 simultaneously cover the first gain waveguide 11 and the second gain waveguide 12 which are close to each other.
  • the material of the pump waveguide 20 includes gallium nitride
  • the material of the gain waveguide component 10 includes erbium-doped gallium nitride.
  • the pumping waveguide 20 can cover all or part of the gain waveguide assembly 10 .
  • the specific situation of this application will continue to be introduced below.
  • FIG. 5 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • Fig. 6 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • the pump waveguide 20 includes a connected first part 21 and a second part 22, and the first part 21 covers the first gain waveguide 11 and the second gain waveguide 12 which are close to each other at the same time. ;
  • the second part 22 covers the rest of the first gain waveguide 11 and the second gain waveguide 12 respectively.
  • the pumping waveguide 20 covers all the first gain waveguides 11 and the second gain waveguides 12 that are close to each other at the same time, but in this embodiment, part of the pumping waveguides 20 simultaneously covers the two close to each other.
  • the first gain waveguide 11 and the second gain waveguide 12 are shown schematically.
  • the pumping waveguide 20 includes a first part 21 and a second part 22 that are connected, and only the first part 21 simultaneously covers the first gain waveguide 11 and the second gain waveguide 12 that are close to each other.
  • the rest of the first gain waveguide 11 and the second gain waveguide 12 are covered by the second part 22, that is, the second part 22 covers the rest of the first gain waveguide 11 and the second gain waveguide 12 respectively.
  • the ends of the first gain waveguide 11 and the second gain waveguide 12 may also need to be physically connected to other devices, so this part of the gain waveguide cannot be connected with other second gain waveguides 12 or first gain waveguides. 11 is covered by the first part 21 at the same time. Therefore, in this embodiment, the second part 22 can be used to respectively cover this part of the first gain waveguide 11 and the second gain waveguide 12 .
  • the first part 21 covers one of the first gain waveguides 11 and one of the second gain waveguides 12 at the same time.
  • the pumping waveguide 20 (that is, the first part 21) covering the first gain waveguide 11 and the second gain waveguide 12 that are close to each other can simultaneously cover one or more first gain waveguides. waveguide 11, and one or more second gain waveguides 12.
  • the first part 21 covers one of the first gain waveguides 11 and one of the second gain waveguides 12 at the same time, which can reduce the signal gap between the first gain waveguide 11 and the second gain waveguide 12. interdependent.
  • FIG. 7 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • the first gain waveguide 11 has an incident end 13
  • the second gain waveguide 12 has an exit end 14, and the incident end 13 and/or the exit end 14 protrude from the pumping waveguide 20.
  • first part 21 is covered, so in this embodiment, the outer periphery of this part of the gain waveguide may not cover the pump waveguide 20, even if the incident end 13 of the first gain waveguide 11 and/or the exit end of the second gain waveguide 12 14 protrudes from the pump waveguide 20, thereby reducing the difficulty of connecting the incident end 13 and/or the exit end 14 to other devices.
  • both the incident end 13 and the exit end 14 protrude from the pumping waveguide 20 for illustration.
  • FIG. 8 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • the first gain waveguide 11 and the second gain waveguide 12 are arranged in a helical shape, and at least part of the second gain waveguide 12 is arranged on the adjacent first gain waveguide 11 between.
  • the incident end 13 and the exit end 14 may be located on the same side or different sides of the helical arrangement.
  • the arrangement shape of the gain waveguide assembly 10 can be limited.
  • the gain waveguide components 10 are arranged in a helical shape, that is, the first gain waveguides 11 and the second gain waveguides 12 are arranged in a helical shape, and at least part of the second gain waveguides 12 are arranged adjacent to each other. between the first gain waveguides 11.
  • the first gain waveguide 11 and the second gain waveguide 12 are actually one waveguide, so the arrangement of the first gain waveguide 11 can be understood as one end outside the spiral shape, and then spirally arranged inward. , and the other end is inside the spiral, from the outer circle to the center.
  • the second gain waveguide 12 is just the opposite.
  • One end of the second gain waveguide 12 is connected to the inside of the first gain waveguide 11 and begins to spiral outward, and at least part of the second gain waveguide 12 is arranged on the adjacent first gain waveguide 11. Between the gain waveguides 11, the other end finally winds to the outside of the helical shape, and detours from the center to the periphery. In this way, the size occupied by the gain waveguide component 10 can be further reduced, and the largest possible waveguide can be placed in the effective area of the chip.
  • the pumping waveguides 20 are also arranged in a helical shape, and there is a distance between adjacent pumping waveguides 20 .
  • the incident end 13 and the exit end 14 are located on different sides of the helical arrangement, as shown in FIG. 8 , the incident end 13 and the exit end 14 Set at 90° so that the incident light and outgoing light are set at 90°.
  • the incident light and the outgoing light can also be arranged at other angles such as 180°, 270°, or the like. The specific angle can be designed according to the needs of the actual product structure.
  • the incident end 13 and the exit end 14 are located on the same side of the helical arrangement, then the incident light and the outgoing light are arranged in parallel.
  • the pump waveguides 20 covering the gain waveguide components 10 in this embodiment are also arranged in a helical shape. And in order to prevent mutual coupling and crosstalk between adjacent pumping waveguides 20 , a space is left between adjacent pumping waveguides 20 . Since this embodiment utilizes the pumping waveguide 20 to cover the first gain waveguide 11 and the second gain waveguide 12 that are close to each other at the same time, even if the pumping waveguide 20 covers two gain waveguides at the same time, the number of pumping waveguides can be reduced. The number of 20 can also reduce the number of intervals between adjacent pumping waveguides 20, thereby reducing the size of the waveguide optical amplifier 1, and finally reducing the size of the chip.
  • the specific distance between adjacent pumping waveguides 20 may be determined according to the size of the waveguide optical amplifier 1 and related parameters of the signal light and the pumping light.
  • FIG. 9 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • a first gain waveguide M111 and a first gain waveguide N112 are provided on opposite sides of the second gain waveguide 12, and the second gain waveguide 12 and the first gain waveguide M111 are arranged on the same
  • the second gain waveguide 12 and the first gain waveguide N112 are arranged in the adjacent pumping waveguide 20; the second gain waveguide 12 and the first gain waveguide
  • the distance between M111 (shown as L1 in FIG. 9 ) is smaller than the distance between the second gain waveguide 12 and the first gain waveguide N112 (shown as L2 in FIG. 9 ).
  • the second gain waveguide 12 is sandwiched between two adjacent first gain waveguides 11 (such as the first gain waveguide M111 and the first gain waveguide N112) during the spiral arrangement process, Between. But the second gain waveguide 12 and the first gain waveguide M111 are covered by the pump waveguide 20 at the same time, and the first gain waveguide N112 is covered with other second gain waveguides 12 . Therefore, in this embodiment, the distance between the second gain waveguide 12 and the first gain waveguide M111 can be made smaller than the distance between the second gain waveguide 12 and the first gain waveguide N112, so that The size of the waveguide optical amplifier 1 is further reduced.
  • the distances between the first gain waveguide 11 and the second gain waveguide 12 covered by adjacent pumping waveguides 20 are equal.
  • FIG. 10 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • the waveguide optical amplifier 1 further includes a coupler 30, and the coupler 30 is connected to the first gain waveguide 11, the second gain waveguide 12, and the pumping waveguide 20 respectively or simultaneously.
  • a coupler 30 can also be added to connect the first gain waveguide 11 and the pumping waveguide 20 .
  • the first gain waveguide 11 has an incident end 13, and the signal light enters the gain waveguide assembly 10 from the incident end 13 of the first gain waveguide 11, so the coupler 30 of this embodiment can be connected to the first gain waveguide 11, and make the signal light entering from the incident end 13 not change after passing through the coupler 30, and continue to be transmitted in the first gain waveguide 11.
  • the coupler 30 of this embodiment is also connected to the pumping waveguide 20, so that the pumping light emitted by the pumping light source 50 can be transmitted into the pumping waveguide 20 through the coupler 30, thereby achieving good transmission of pumping light and signals. .
  • FIG. 11 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • the pump waveguide 20 has a light incident end 23 and a reflective end 24 oppositely arranged
  • the waveguide optical amplifier 1 further includes a reflective member 40, and the reflective member 40 is arranged on the reflective end 24, used to reflect the pump light arriving there.
  • the pumping waveguide 20 also has two opposite ends, for example, the pumping waveguide 20 has a light incident end 23 and a reflection end 24 oppositely set, wherein the light incident end 23 is used to allow the pumping light to enter the pump.
  • the end of the Pu waveguide 20, and the reflective end 24 arranged opposite to it is used for reflection.
  • the pumping light When the pumping light enters the pumping waveguide 20 from the light incident end 23 , it will be transmitted in the pumping waveguide 20 and amplify the signal light in the gain waveguide component 10 . But not all the pumping light will be amplified, so some of the pumping light will always be transmitted in the pumping waveguide 20, when this part of the pumping light arriving here is transmitted to the reflection end 24, in this embodiment In this way, a reflector 40 can be provided on the reflective end 24, so that this part of the excess pump light can be retransmitted from the reflective end 24 to the light incident end 23 again, and the pump light arriving here can be reused, reducing the The energy loss improves the amplification effect of the waveguide optical amplifier 1 .
  • FIG. 12 is a schematic diagram of a waveguide optical amplifier in another embodiment of the present application.
  • the waveguide optical amplifier 1 further includes a pumping light source 50, the pumping light source 50 is close to the light-incident end 23, and the light of the pumping light source 50 passes from the light-incident end 23 to The coupler 30 enters the pump waveguide 20.
  • bidirectional pumping is usually used, that is, a pumping light source 50 is set from the incident end 13 of the gain waveguide assembly 10, and a pumping light source 50 is set at the outgoing end 14, so that the pumping light source 50 at the incident end 13
  • the transmission direction of the emitted light in the pumping waveguide 20 is the same as that of the signal light.
  • the transmission direction of the light emitted by the pumping light source 50 at the output end 14 in the pumping waveguide 20 is opposite to the transmission direction of the signal light, so as to achieve the purpose of a bidirectional waveguide.
  • This embodiment also adopts bidirectional pumping, but since this embodiment adopts a new waveguide optical amplifier 1 and designs a new structure, this embodiment only needs to use the pumping light source 50, and the pumping light source 50 Two-way pumping can be realized by setting it close to the light incident end 23.
  • the specific principle is as follows: because the pumping waveguide 20 in this embodiment covers the first gain waveguide 11 and the second gain waveguide 12 that are close to each other at the same time, and The transmission directions of the signal light in the first gain waveguide 11 and the second gain waveguide 12 are opposite.
  • the pumping light emitted by the pumping light source 50 enters the pumping waveguide 20 from the light incident end 23 and propagates, the light is equivalent to passing through the first gain waveguide 11 and the second gain waveguide 12 at the same time. And for the first gain waveguide 11, the transmission direction of the signal light and the pump light are the same. For the second gain waveguide 12, the transmission directions of the signal light and the pump light are opposite. Therefore, this embodiment only needs one pumping light source 50 to achieve bidirectional pumping, which reduces the number of pumping light sources 50 and reduces the cost and size of the waveguide optical amplifier 1 .
  • FIG. 13 is a schematic cross-sectional view of a waveguide optical amplifier in another embodiment of the present application.
  • the waveguide optical amplifier 1 further includes a substrate 60, the gain waveguide component 10 and the pump waveguide 20 are both disposed on the substrate 60, and the gain waveguide component 10 and the The pumping waveguide 20 is also arranged between the substrates 60 .
  • the gain waveguide assembly 10 and the pump waveguide 20 can be disposed on the substrate 60 .
  • the substrate 60 is a component carrying the gain waveguide assembly 10 and the pumping waveguide 20 .
  • the pumping waveguide 20 is also provided between the gain waveguide component 10 and the substrate 60 , that is, the pumping waveguide 20 completely covers the surroundings of the gain waveguide component 10 .
  • the waveguide optical amplifier 1 at this time can be considered as a part of the chip, that is, the waveguide optical amplifier 1 is integrated in the on the chip, or it can also be understood as designing a part of the chip area as a waveguide optical amplifier 1 .
  • the substrate 60 and the pumping waveguide 20 are integrally structured.
  • the coupler 30 and/or the pump light source 50 are also disposed on the substrate 60 .

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

本申请提供了波导光放大器，包括增益波导组件与泵浦波导。增益波导组件包括弯折连接的第一增益波导与第二增益波导，至少部分第一增益波导靠近至少部分第二增益波导，信号在第一增益波导内的传输方向与在第二增益波导内的传输方向相反。泵浦波导包覆至少部分增益波导组件，且至少部分泵浦波导同时包覆相互靠近的第一增益波导与第二增益波导。本申请利用泵浦波导同时包覆相互靠近的第一增益波导与第二增益波导可减少泵浦波导的长度及相邻的泵浦波导之间间距的数量，还可减少包覆在一起的增益波导之间的间距，从而减少波导光放大器的尺寸。由于泵浦波导同时包覆了传输方向相反的增益波导，单个泵浦光源也可实现双向泵浦，减小光放大器的尺寸。

Description

波导光放大器 技术领域
本申请属于光放大器技术领域，具体涉及波导光放大器。
背景技术
光放大器是基础光学器件，也是未来光器件小型化，集成化的重要光学器件之一，现广泛应用于光器件互连及光通信网络中。但是目前主流光放大器的尺寸较大，无法满足光放大器小型化、集成化的市场需求及技术趋势。
发明内容
鉴于此，本申请提供了一种波导光放大器，包括：
增益波导组件，包括弯折连接的第一增益波导与第二增益波导，所述第一增益波导具有入射端，所述第二增益波导具有出射端，至少部分所述第一增益波导靠近至少部分所述第二增益波导，信号在所述第一增益波导内的传输方向与在所述第二增益波导内的传输方向相反；
泵浦波导，包覆至少部分所述增益波导组件，且至少部分所述泵浦波导同时包覆相互靠近的所述第一增益波导与所述第二增益波导。
其中，所述增益波导组件用于传输信号光，所述泵浦波导用于传输泵浦光。
其中，所述增益波导组件的材质包括掺饵氮化镓。
其中，所述泵浦波导的材质包括氮化镓及其他III族氮化物。
其中，所述泵浦波导包括相连接的第一部分与第二部分，所述第一部分同时包覆相互靠近的所述第一增益波导与所述第二增益波导；第二部分分别包覆其余的所述第一增益波导与所述第二增益波导。
其中，所述第一部分同时包覆一个所述第一增益波导与一个所述第二增益波导。
其中，所述第一增益波导与所述第二增益波导均成螺旋状排布设置，且至少部分所述第二增益波导设于相邻的所述第一增益波导之间，所述入射端与所述出射端可位于螺旋状排布的同侧或不同侧。
其中，所述泵浦波导也呈螺旋状排布设置，且相邻的所述泵浦波导之间具有间距。
其中，所述第二增益波导的相对两侧设有第一增益波导M、以及第一增益波导N，所述第二增益波导与所述第一增益波导M设于相同的所述泵浦波导内，所述第二增益波导与所述第一增益波导N设于相邻的所述泵浦波导内；所述第二增益波导与所述第一增益波导M之间的距离小于所述第二增益波导与所述第一增益波导N之间的距离。
其中，当所述入射端与所述出射端位于螺旋状排布的同侧时，所述入射端与所述出射端呈90°、180°、或270°设置，以使入射光与出射光垂直设置；当所述入射端与所述出射端位于螺旋状排布的同侧时，所述入射光与所述出射光平行设置。
其中，相邻的所述泵浦波导包覆的所述第一增益波导与所述第二增益波导之间的距离相等。
其中，所述入射端和/或所述出射端可凸出于所述泵浦波导。
其中，所述泵浦波导具有相对设置的入光端与反射端，所述波导光放大器还包括反射件，所述反射件设于所述反射端上，用于反射到达此处的所述泵浦光。
其中，所述波导光放大器还包括耦合器，所述耦合器分别或同时连接所述第一增益波导、所述第二增益波导、所述泵浦波导。
其中，所述泵浦波导具有入光端，所述波导光放大器还包括泵浦光源，所述泵浦光源靠近所述入光端，且所述泵浦光源的泵浦光线从所述入光端的所述耦合器进入所述泵浦波导。
其中，所述入射端处的所述泵浦光源发出的光线在所述泵浦波导内的传输方向与信号光的传输方向相同；在所述出射端处的所述泵浦光源发出的光线在所述泵浦波导内的传输方向与信号光的传输方向相反。
其中，所述波导光放大器还包括衬底，所述增益波导组件与所述泵浦波导均设于所述衬底上，且所述增益波导组件与所述衬底之间还设有所述泵浦波导。
其中，所述衬底与所述泵浦波导可为一体式结构。
其中，所述波导光放大器还包括耦合器与泵浦光源，所述耦合器和/或所述泵浦光源也设于所述衬底上。
附图说明
为了更清楚地说明本申请实施方式中的技术方案，下面将对本申请实施方式中所需要使用的附图进行说明。
图1为本申请一实施方式中波导光放大器的示意图。
图2为图1中沿A-A方向的截面示意图。
图3为本申请另一实施方式中波导光放大器的示意图。
图4为本申请又一实施方式中波导光放大器的示意图。
图5为本申请又一实施方式中波导光放大器的示意图。
图6为本申请又一实施方式中波导光放大器的示意图。
图7为本申请又一实施方式中波导光放大器的示意图。
图8为本申请又一实施方式中波导光放大器的示意图。
图9为本申请又一实施方式中波导光放大器的示意图。
图10为本申请又一实施方式中波导光放大器的示意图。
图11为本申请又一实施方式中波导光放大器的示意图。
图12为本申请又一实施方式中波导光放大器的示意图。
图13为本申请另一实施方式中波导光放大器的截面示意图。
标号说明：
波导光放大器-1，增益波导组件-10，第一增益波导-11，第一增益波导M-111，第一增益波导N-112，第二增益波导-12，入射端-13，出射端-14，泵浦波导-20，第一部分-21，第二部分-22，入光端-23，反射端-24，耦合器-30，反射件-40，泵浦光源-50，衬底-60。
具体实施方式
以下是本申请的优选实施方式，应当指出，对于本技术领域的普通技术人员来说，在不脱离本申请原理的前提下，还可以做出若干改进和润饰，这些改进和润饰也视为本申请的保护范围。
在介绍本申请的技术方案之前，再详细介绍下相关技术中的技术问题。
光放大器是高速光通信系统中的关键器件，也是未来光器件小型化，集成化的重要光学器件之一。光放大器包括光纤放大器、波导光放大器及其他类型的光放大器。其中，光纤放大器采用稀土掺杂光纤作为放大介质的载体。但由于光纤及分立光器件的尺寸和体积较大，难以满足光模块小型化集成的需求，只能作为独立的子系统进行使用。可替代光纤放大器的波导光放大器具有小型化的特点，可以集成到芯片上，目前已受到越来越多学者的关注与研究。
另外，波导光放大器根据泵浦光和信号光传输方向的区别可以分为正向泵浦、反向泵浦和双向泵浦三种方式。其中，正向泵浦指的是泵浦光和信号光同方向打入，即传输方向相同，反向泵浦指的是泵浦光和信号光从相反的方向打入，即传输方向相反。而双向泵浦则是从正向反向各打入一束泵浦光，使得一部分信号光和泵浦光的传输方向相同，一部分信号光和泵浦光的传输信号相反。并且，正向泵浦的噪声系数较小，但是饱和功率低，不利于高输出功率的应用。而反向泵浦的噪声系数大，但是饱和功率高。双向泵浦则可同时兼具两者的优点，即噪声系数小，饱和功率高。
波导光放大器从结构上来分可以分为芯层和围绕在其外面的包层。通常信号光主要在芯层中传播，作为光放大器使用的波导，根据泵浦光所在的位置，可分为芯层泵浦和包层泵浦两种。其中包层泵浦可以容纳更多的泵浦光，因此具有更高的泵浦耦合效率。
由于相邻的波导接触时会存在耦合串扰现象，因此相邻的波导必须要分开一定的间距以保证相互之间不产生影响。由于泵浦光所在的包层波导通常比较宽，间距就必须比较大，导致波导光放大器的尺寸较大，不利于缩小芯片尺寸。
鉴于此，为了解决上述问题，本申请提供了一种新型的波导光放大器。请一并参考图1-图4，图1为本申请一实施方式中波导光放大器的示意图。图2为图1中沿A-A方向的截面示意图。图3为本申请另一实施方式中波导光放大器的示意图。图4为本申请又一实施方式中波导光放大器的示意图。本实施方式提供了一种波导光放大器1，具体包括增益波导组件10与泵浦波导20。其中，增益波导组件10包括弯折连接的第一增益波导11与第二增益波导12，所述第一增益波导11具有入射端13，所述第二增益波导12具有出射端14，至少部分所述第一增益波导11靠近至少部分所述第二增益波导12，信号在所述第一增益波导11内的传输方向与在所述第二增益波导12内的传输方向相反。泵浦波导20包覆至少部分所述增益波导组件10，且至少部分所述泵浦波导20同时包覆相互靠近的所述第一增益波导11与所述第二增益波导12。
本实施方式提供的波导光放大器1包括增益波导组件10，其中增益波导组件10的作用是传输信号，即增益波导组件10也可以看做是芯层。增益波导组件10并不是由一种增益波导组成，而是由至少两种增益波导组成，即弯折连接的第一增益波导11与第二增益波导12。或者也可以理解为增益波导组件10是一根增益波导，只不过为了便于区分，将该波导从弯折处根据其功能的不同进行了人为的命名区分。例如信号在所述第一增益波导11内的传输方向与在所述第二增益波导12内的传输方向相反，因此根据信号传播的方向的相 同与否对增益波导进行了区分。即第一增益波导11与第二增益波导12为一体式结构。
本实施方式将增益波导组件10分成弯折连接的第一增益波导11与第二增益波导12，同时还使至少部分所述第一增益波导11靠近至少部分所述第二增益波导12，即将一根较长的增益波导弯折成两段增益波导，从而减少增益波导组件10所占的尺寸。并且这样弯折设置后，信号在所述第一增益波导11内的传输方向与在所述第二增益波导12内的传输方向相反(如图1中D1方向所示)，为后续泵浦波导20与泵浦光的设置打下了基础。
本实施方式提供的波导光放大器1还包括泵浦波导20，使泵浦波导20包覆所述增益波导组件10。泵浦波导20的作用是用于包覆并保护增益波导组件10，因此泵浦波导20可以看做是包层。并且泵浦波导20还用于传输泵浦光，即信号光是在增益波导组件10内传输，而泵浦光则在泵浦波导20内传输，因此本申请提供的波导光放大器1可以看做是包层泵浦。泵浦光的作用是对在增益波导组件10内的信号光提供额外的能量从而使信号光可以进行放大。
另外，本实施方式还可使至少部分所述泵浦波导20同时包覆相互靠近的所述第一增益波导11与所述第二增益波导12。现有技术中泵浦波导20只包覆一个增益波导(第一增益波导11或第二增益波导12)，并且为了防止相邻的波导接触时会存在耦合串扰现象，相邻的泵浦波导20之间会存在间距。而本申请利用泵浦波导20同时包覆相互靠近的所述第一增益波导11与所述第二增益波导12，即使泵浦波导20同时包覆两个或多个增益波导，因此可减少泵浦波导20的长度，还可减少相邻的泵浦波导20之间间距的数量及同时包覆在泵浦波导中第一增益波导11与第二增益波导12之间的间距，从而减少波导光放大器1的尺寸，最终减小芯片的尺寸。由于泵浦波导20同时包覆了传输方向相反的增益波导，单个泵浦光源也可实现双向泵浦，进一步减小光放大器的1尺寸，达到用户的需求。本实施方式以全部泵浦波导20同时包覆相互靠近的所述第一增益波导11与所述第二增益波导12进行示意。
可选地，泵浦波导20的材质包括氮化镓，增益波导组件10的材质包括掺饵氮化镓。
可选地，本实施方式可使泵浦波导20覆盖全部增益波导组件10或者部分增益波导组件10。具体情况本申请将在下文继续介绍。
请一并参考图5-图6，图5为本申请又一实施方式中波导光放大器的示意图。图6为本申请又一实施方式中波导光放大器的示意图。本实施方式中，所述泵浦波导20包括相连接的第一部分21与第二部分22，所述第一部分21同时包覆相互靠近的所述第一增益波导 11与所述第二增益波导12；第二部分22分别包覆其余的所述第一增益波导11与所述第二增益波导12。
上述实施方式以泵浦波导20同时包覆全部相互靠近的所述第一增益波导11与所述第二增益波导12进行示意，而在本实施方式中以部分泵浦波导20同时包覆相互靠近的所述第一增益波导11与所述第二增益波导12进行示意。例如，泵浦波导20包括相连接的第一部分21与第二部分22，只有第一部分21同时包覆相互靠近的所述第一增益波导11与所述第二增益波导12。而其余的第一增益波导11与第二增益波导12则由第二部分22来进行包覆，即第二部分22分别包覆其余的所述第一增益波导11与所述第二增益波导12。
在本实施方式中，第一增益波导11与第二增益波导12的端部可能还需要与其他器件进行物理连接，因此导致这部分增益波导无法与其他的第二增益波导12或第一增益波导11同时被第一部分21所包覆。因此，本实施方式便可采用第二部分22来对这部分的第一增益波导11与第二增益波导12分别进行包覆。
请再次参考图6，本实施方式中，所述第一部分21同时包覆一个所述第一增益波导11与一个所述第二增益波导12。
在本实施方式中，同时包覆相互靠近的所述第一增益波导11与所述第二增益波导12的泵浦波导20(即第一部分21)，可同时包覆一个或多个第一增益波导11、及一个或多个第二增益波导12。在本实施方式中，所述第一部分21同时包覆一个所述第一增益波导11与一个所述第二增益波导12，可减小第一增益波导11与第二增益波导12之间信号的相互影响。
请一并参考图7，图7为本申请又一实施方式中波导光放大器的示意图。本实施方式中，所述第一增益波导11具有入射端13，所述第二增益波导12具有出射端14，所述入射端13和/或所述出射端14凸出于所述泵浦波导20。
从上述内容可知，第一增益波导11的一端与第二增益波导12的一端可能由于需要与其他部件进行物理连接或者电连接，因此这部分第一增益波导11与第二增益波导12无法同时被第一部分21所包覆，所以在本实施方式中，对于这部分增益波导的外周缘可不覆盖泵浦波导20，即使第一增益波导11的入射端13和/或第二增益波导12的出射端14凸出于泵浦波导20，从而降低入射端13和/或出射端14与其他器件的连接难度。
可选地，本实施方式以所述入射端13和所述出射端14均凸出于所述泵浦波导20进行示意。
请一并参考图8，图8为本申请又一实施方式中波导光放大器的示意图。本实施方式中，所述第一增益波导11与所述第二增益波导12均成螺旋状排布设置，且至少部分所述第二增益波导12设于相邻的所述第一增益波导11之间。所述入射端13与所述出射端14可位于螺旋状排布的同侧或不同侧。
在本实施方式中，可对增益波导组件10的排布形状进行限定。例如增益波导组件10成螺旋状排布设置，即所述第一增益波导11与所述第二增益波导12均成螺旋状排布设置，且至少部分所述第二增益波导12设于相邻的所述第一增益波导11之间。从上述内容可知，第一增益波导11与第二增益波导12实际上为一根波导，因此第一增益波导11的排布可以理解为一端在螺旋状的外部，然后向内呈螺旋状排布，另一端在螺旋状的内部，从外围绕到中心。而第二增益波导12正好相反，第二增益波导12的一端在内部连接第一增益波导11的内部开始向外螺旋，并且至少部分所述第二增益波导12设于相邻的所述第一增益波导11之间，最终另一端绕到螺旋状的外部，从中心绕道外围。这样可进一步降低增益波导组件10所占的尺寸，在芯片的有效面积内放置尽可能场的波导。
可选地，请再次参考图8，本实施方式中，所述泵浦波导20也呈螺旋状排布设置，且相邻的所述泵浦波导20之间具有间距。
可选地，在本实施方式中，以所述入射端13与所述出射端14位于螺旋状排布的不同侧进行示意，如图8所示，所述入射端13与所述出射端14呈90°设置，从而使得入射光与出射光成90°设置。当然了，在其他方式中，当所述入射端13与所述出射端14位于螺旋状排布的不同侧时，入射光与出射光还可以呈180°，270°等其他角度设置。具体地角度可根据实际产品结构的需要来进行设计。另外，当所述入射端13与所述出射端14位于螺旋状排布的同侧时，此时即为入射光与出射光平行设置。
从上述内容可知，由于增益波导组件10呈螺旋状排布设置，因此本实施方式中包覆增益波导组件10的泵浦波导20也呈螺旋状排布设置。并且了防止相邻的泵浦波导20之间相互耦合串扰现象，因此是相邻的所述泵浦波导20之间留有间距。由于本实施方式利用泵浦波导20同时包覆相互靠近的所述第一增益波导11与所述第二增益波导12，即使泵浦波导20同时包覆两个增益波导，因此可减少泵浦波导20的数量，还可减少相邻的泵浦波导20之间间距的数量，从而减少波导光放大器1的尺寸，最终减小芯片的尺寸。
可选地，至于相邻的泵浦波导20之间具体的间距为多少可根据波导光放大器1的尺寸、信号光与泵浦光的相关参数来决定。
请一并参考图9，图9为本申请又一实施方式中波导光放大器的示意图。本实施方式中，所述第二增益波导12的相对两侧设有第一增益波导M111、以及第一增益波导N112，所述第二增益波导12与所述第一增益波导M111设于相同的所述泵浦波导20内，所述第二增益波导12与所述第一增益波导N112设于相邻的所述泵浦波导20内；所述第二增益波导12与所述第一增益波导M111之间的距离(如图9中L1所示)小于所述第二增益波导12与所述第一增益波导N112之间的距离(如图9中L2所示)。
在本实施方式中，由于第二增益波导12在绕螺旋状排布的过程中是夹设于相邻的两个第一增益波导11(例如第一增益波导M111与第一增益波导N112)之间的。但第二增益波导12只与第一增益波导M111被泵浦波导20同时包覆，第一增益波导N112则是与其他的第二增益波导12被包覆。因此，在本实施方式中可使所述第二增益波导12与所述第一增益波导M111之间的距离小于所述第二增益波导12与所述第一增益波导N112之间的距离，从而进一步减小波导光放大器1的尺寸。
可选地，相邻的泵浦波导20包覆的第一增益波导11与第二增益波导12之间的距离相等。
请一并参考图10，图10为本申请又一实施方式中波导光放大器的示意图。本实施方式中，所述波导光放大器1还包括耦合器30，所述耦合器30分别或同时连接所述第一增益波导11、所述第二增益波导12、所述泵浦波导20。
在本实施方式中，还可增设耦合器30将耦合器30连接第一增益波导11与泵浦波导20。从上述内容可知，第一增益波导11具有入射端13，信号光是从第一增益波导11的入射端13进入增益波导组件10中的，因此本实施方式的耦合器30可以连接第一增益波导11，并使从入射端13进入的信号光经过耦合器30之后不会发生变化，继续在第一增益波导11内传输。
另外，本实施方式的耦合器30还连接泵浦波导20，这样可使泵浦光源50发出的泵浦光线经过耦合器30可传输到泵浦波导20内，从而实现泵浦光与信号良好传输。
请一并参考图11，图11为本申请又一实施方式中波导光放大器的示意图。本实施方式中，所述泵浦波导20具有相对设置的入光端23与反射端24，所述波导光放大器1还包括反射件40，所述反射件40设于所述反射端24上，用于反射到达此处的所述泵浦光。
在本实施方式中，泵浦波导20同样具有相对设置的两端，例如泵浦波导20具有相对设置的入光端23与反射端24，其中入光端23是用于使泵浦光进入泵浦波导20的端部， 而与之相对设置的反射端24则是用于反射的。
当泵浦光从入光端23进入泵浦波导20后，会在泵浦波导20内进行传输，并对在增益波导组件10内的信号光线进行放大。但是并不是所有的泵浦光均会进行放大，所以就会有部分泵浦光一直在泵浦波导20内进行传输，当这部分到达此处的泵浦光传输到反射端24时，本实施方式可在反射端24上设置反射件40，从而让这部分多余泵浦光重新从反射端24向入光端23再传输一次，便可将到达此处的泵浦光重新利用起来，降低了能量损耗，提高了波导光放大器1的放大效果。
请一并参考图12，图12为本申请又一实施方式中波导光放大器的示意图。本实施方式中，所述波导光放大器1还包括泵浦光源50，所述泵浦光源50靠近所述入光端23，且所述泵浦光源50的光线从所述入光端23的所述耦合器30进入所述泵浦波导20。
在现有技术中通常采用双向泵浦，即从增益波导组件10的入射端13设置一个泵浦光源50，再在出射端14设置一个泵浦光源50，这样入射端13处的泵浦光源50发出的光线在泵浦波导20内的传输方向与信号光的传输方向相同。而在出射端14处的泵浦光源50发出的光线在泵浦波导20内的传输方向与信号光的传输方向相反，从而实现双向波导的目的。
本实施方式同样是采用双向泵浦，但由于本实施方式采用了一个新的波导光放大器1，设计了一个新型结构，因此本实施方式只需要使用泵浦光源50，并使该泵浦光源50靠近入光端23设置即可实现双向泵浦，具体原理如下：因为本实施方式中的泵浦波导20同时包覆相互靠近的所述第一增益波导11与所述第二增益波导12，并且在第一增益波导11与第二增益波导12内的信号光的传输方向相反。因此，当泵浦光源50发出的泵浦光从入光端23进入所述泵浦波导20内并进行传播时，该光线相当于同时经过第一增益波导11与第二增益波导12。并且对于第一增益波导11来说，信号光与泵浦光的传输方向相同。对于第二增益波导12来说，信号光与泵浦光的传输方向相反。因此本实施方式只需要一个泵浦光源50便可实现双向泵浦的目的，减小了泵浦光源50的数量，降低了波导光放大器1的成本及尺寸。
请一并参考图13，图13为本申请另一实施方式中波导光放大器的截面示意图。本实施方式中，所述波导光放大器1还包括衬底60，所述增益波导组件10与所述泵浦波导20均设于所述衬底60上，且所述增益波导组件10与所述衬底60之间还设有所述泵浦波导20。
在本实施方式中，可将增益波导组件10与泵浦波导20设于衬底60上。其中衬底60为承载增益波导组件10与泵浦波导20的部件。并且且所述增益波导组件10与所述衬底60之间还设有所述泵浦波导20，即泵浦波导20将增益波导组件10的四周全面包覆了起来。
可选地，当衬底上的同一个区域除了增益波导组件10与泵浦波导20还有其他功能器件时，此时的波导光放大器1可以认为是芯片的一部分，即将波导光放大器1集成在了芯片上，或者也可以理解为将芯片的一部分区域设计成波导光放大器1。
可选地，所述衬底60与所述泵浦波导20为一体式结构。可选地，耦合器30和/或泵浦光源50也设于衬底60上。
以上对本申请实施方式所提供的内容进行了详细介绍，本文对本申请的原理及实施方式进行了阐述与说明，以上说明只是用于帮助理解本申请的方法及其核心思想；同时，对于本领域的一般技术人员，依据本申请的思想，在具体实施方式及应用范围上均会有改变之处，综上所述，本说明书内容不应理解为对本申请的限制。

Claims (19)

  1. 一种波导光放大器，其特征在于，包括：
    增益波导组件，包括弯折连接的第一增益波导与第二增益波导，所述第一增益波导具有入射端，所述第二增益波导具有出射端，至少部分所述第一增益波导靠近至少部分所述第二增益波导，信号在所述第一增益波导内的传输方向与在所述第二增益波导内的传输方向相反；
    泵浦波导，包覆至少部分所述增益波导组件，且至少部分所述泵浦波导同时包覆相互靠近的所述第一增益波导与所述第二增益波导。
  2. 如权利要求1所述的波导光放大器，其特征在于，所述增益波导组件用于传输信号光，所述泵浦波导用于传输泵浦光。
  3. 如权利要求1所述的波导光放大器，其特征在于，所述增益波导组件的材质包括掺饵氮化镓及其他III族氮化物。
  4. 如权利要求1所述的波导光放大器，其特征在于，所述泵浦波导的材质包括氮化镓及其他III族氮化物。
  5. 如权利要求1所述的波导光放大器，其特征在于，所述泵浦波导包括相连接的第一部分与第二部分，所述第一部分同时包覆相互靠近的所述第一增益波导与所述第二增益波导；第二部分分别包覆其余的所述第一增益波导与所述第二增益波导。
  6. 如权利要求5所述的波导光放大器，其特征在于，所述第一部分同时包覆一个所述第一增益波导与一个所述第二增益波导。
  7. 如权利要求1所述的波导光放大器，其特征在于，所述第一增益波导与所述第二增益波导均成螺旋状排布设置，且至少部分所述第二增益波导设于相邻的所述第一增益波导之间，所述入射端与所述出射端可位于螺旋状排布的同侧或不同侧。
  8. 如权利要求7所述的波导光放大器，其特征在于，所述泵浦波导也呈螺旋状排布设置，且相邻的所述泵浦波导之间具有间距。
  9. 如权利要求7所述的波导光放大器，其特征在于，所述第二增益波导的相对两侧设有第一增益波导M、以及第一增益波导N，所述第二增益波导与所述第一增益波导M设于相同的所述泵浦波导内，所述第二增益波导与所述第一增益波导N设于相邻的所述泵浦波导内；所述第二增益波导与所述第一增益波导M之间的距离小于所述第二增益波导与所述第一增益波导N之间的距离。
  10. 如权利要求7所述的波导光放大器，其特征在于，当所述入射端与所述出射端位于螺旋状排布的同侧时，所述入射端与所述出射端呈90°、180°、或270°设置，以使入射光与出射光垂直设置；当所述入射端与所述出射端位于螺旋状排布的同侧时，所述入射光与所述出射光平行设置。
  11. 如权利要求1所述的波导光放大器，其特征在于，相邻的所述泵浦波导包覆的所述第一增益波导与所述第二增益波导之间的距离相等。
  12. 如权利要求1所述的波导光放大器，其特征在于，所述入射端和/或所述出射端凸出于所述泵浦波导。
  13. 如权利要求1所述的波导光放大器，其特征在于，所述泵浦波导具有相对设置的入光端与反射端，所述波导光放大器还包括反射件，所述反射件设于所述反射端上，用于反射到达此处的所述泵浦光。
  14. 如权利要求1所述的波导光放大器，其特征在于，所述波导光放大器还包括耦合器，所述耦合器分别或同时连接所述第一增益波导、所述第二增益波导、所述泵浦波导。
  15. 如权利要求14所述的波导光放大器，其特征在于，所述泵浦波导具有入光端，所述波导光放大器还包括泵浦光源，所述泵浦光源靠近所述入光端，且所述泵浦光源的泵浦 光线从所述入光端的所述耦合器进入所述泵浦波导。
  16. 如权利要求15所述的波导光放大器，其特征在于，所述入射端处的所述泵浦光源发出的光线在所述泵浦波导内的传输方向与信号光的传输方向相同；在所述出射端处的所述泵浦光源发出的光线在所述泵浦波导内的传输方向与信号光的传输方向相反。
  17. 如权利要求1-16任一项所述的波导光放大器，其特征在于，所述波导光放大器还包括衬底，所述增益波导组件与所述泵浦波导均设于所述衬底上，且所述增益波导组件与所述衬底之间还设有所述泵浦波导。
  18. 如权利要求17所述的波导光放大器，其特征在于，所述衬底与所述泵浦波导为一体式结构。
  19. 如权利要求17所述的波导光放大器，其特征在于，所述波导光放大器还包括耦合器与泵浦光源，所述耦合器和/或所述泵浦光源也设于所述衬底上。
PCT/CN2022/094892 2021-05-28 2022-05-25 波导光放大器 WO2022247851A1 (zh)

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
CN202110593593.7A CN113359232A (zh) 2021-05-28 2021-05-28 波导光放大器
CN202121190000.4U CN215813433U (zh) 2021-05-28 2021-05-28 波导光放大器
CN202121190000.4 2021-05-28
CN202110593593.7 2021-05-28

Publications (1)

Publication Number Publication Date
WO2022247851A1 true WO2022247851A1 (zh) 2022-12-01

Family

ID=84229500

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/CN2022/094892 WO2022247851A1 (zh) 2021-05-28 2022-05-25 波导光放大器

Country Status (1)

Country Link
WO (1) WO2022247851A1 (zh)

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20030002771A1 (en) * 2001-06-01 2003-01-02 Jds Uniphase Corporation Integrated optical amplifier
CN1752778A (zh) * 2005-10-18 2006-03-29 电子科技大学 S形铒镱共掺磷酸盐高增益光波导、光波导激光器和光波导放大器
CN105428982A (zh) * 2015-12-14 2016-03-23 中国科学院西安光学精密机械研究所 半导体直接泵浦光纤激光器
US20190020169A1 (en) * 2017-07-13 2019-01-17 Dicon Fiberoptics, Inc. Solid-state optical amplifier chip with improved optical pumping
CN113359232A (zh) * 2021-05-28 2021-09-07 珠海庞纳微半导体科技有限公司 波导光放大器

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20030002771A1 (en) * 2001-06-01 2003-01-02 Jds Uniphase Corporation Integrated optical amplifier
CN1752778A (zh) * 2005-10-18 2006-03-29 电子科技大学 S形铒镱共掺磷酸盐高增益光波导、光波导激光器和光波导放大器
CN105428982A (zh) * 2015-12-14 2016-03-23 中国科学院西安光学精密机械研究所 半导体直接泵浦光纤激光器
US20190020169A1 (en) * 2017-07-13 2019-01-17 Dicon Fiberoptics, Inc. Solid-state optical amplifier chip with improved optical pumping
CN113359232A (zh) * 2021-05-28 2021-09-07 珠海庞纳微半导体科技有限公司 波导光放大器

Similar Documents

Publication Publication Date Title
US4549782A (en) Active optical fiber tap
CN100492079C (zh) 光波导模块
US7548669B2 (en) Optical gate array device
CN101535859B (zh) 光学连接组件
US5007698A (en) Optical fiber amplifier/multiplexer
US20120148257A1 (en) Optical transceiver using single-wavelength communication
WO2017152721A1 (zh) 光耦合连接器、光耦合系统及波导耦合方法
US6467969B1 (en) Article comprising a multimode optical fiber coupler
US5475777A (en) Optical device with a pig tail optical fiber and its production method
US20220276454A1 (en) Optical receiving engine based on planar waveguide chip
US7778502B2 (en) Optical transmission assembly
CN103487899B (zh) 一种单纤双向光收发器件
US6330117B1 (en) Optical isolator module and optical amplifier using the same
WO2022247851A1 (zh) 波导光放大器
CN113359232A (zh) 波导光放大器
CN215813433U (zh) 波导光放大器
US7546012B2 (en) Waveguide system with diffracting structure
WO2021026774A1 (zh) 一种多通道并行双向器件耦合装置
JPS60214316A (ja) 双方向伝送用光モジユ−ル
CN201122792Y (zh) 一种集成光隔离器的半导体激光器
WO2020000776A1 (zh) 一种光学装置
US20080050067A1 (en) Optical gate array device
CN103326784A (zh) 光通讯系统
CN218040189U (zh) 桥连式大模场光纤结构以及光纤放大器
KR101265754B1 (ko) 광 도파로 장치

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 22810575

Country of ref document: EP

Kind code of ref document: A1

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 22810575

Country of ref document: EP

Kind code of ref document: A1

32PN Ep: public notification in the ep bulletin as address of the adressee cannot be established

Free format text: NOTING OF LOSS OF RIGHTS PURSUANT TO RULE 112(1) EPC (EPO FORM 1205A DATED 11.06.2024)